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Featured researches published by P. Kubes.


Plasma Physics and Controlled Fusion | 2012

Experimental study of the structure of the plasma-current sheath on the PF-1000 facility

Viacheslav I. Krauz; K Mitrofanov; M. Scholz; M. Paduch; L. Karpinski; Ewa Zielinska; P. Kubes

The results of studies of the plasma-current sheath structure on the PF-1000 facility in the stage close to the instant of pinch formation are presented. The measurements were performed using various modifications of the calibrated magnetic probes. Studies of the influence of the probe shape and dimensions on the measurements accuracy were done. The current flowing in the converging sheath at a distance of 40 mm from the axis of the facility electrodes was measured. In the optimal operating modes, this current is equal to the total discharge current, which indicates the high efficiency of current transportation toward the axis. In such shots a compact high-quality sheath forms with shock wave in front of the magnetic piston. It is shown that the neutron yield depends on the current compressed onto the axis. This dependence agrees well with the known scaling, Yn ~ I4. The use of the total discharge current in constructing the current scaling, especially for facilities with a large stored energy, is unjustified.


Surface Review and Letters | 2002

ABLATION OF POLY(METHYL METHACRYLATE) BY A SINGLE PULSE OF SOFT X-RAYS EMITTED FROM Z-PINCH AND LASER-PRODUCED PLASMAS

L. Juha; J. Krása; A. Präg; Andrea Cejnarova; Dagmar Chvostova; K. Rohlena; K. Jungwirth; J. Kravarik; P. Kubes; Yu. L. Bakshaev; A. S. Chernenko; V. D. Korolev; V. I. Tumanov; M. I. Tumanov; A. Bernardinello; J. Ullschmied; F. P. Boody

The efficiency of ablation induced in poly(methyl methacrylate) (PMMA) by single soft X-ray pulses emitted from Z-pinch and laser-produced plasmas was determined. X-ray ablation of PMMA was found to be less efficient than that of teflon (PTFE). Nonthermal effects of the radiation on the polymer structure play a key role in the mechanisms of the ablation, i.e. the ablation can be explained by the formation of radiation-chemical scissions of the polymer chain followed by blowoff of low-molecular fragment fluid into the vacuum. The most promising application of this phenomenon seems to be micropatterning/micromachining.


Laser and Particle Beams | 2007

The influence of an intense laser beam interaction with preformed plasma on the characteristics of emitted ion streams

L. Láska; J. Badziak; S. Gammino; K. Jungwirth; A. Kasperczuk; J. Krása; E. Krouský; P. Kubes; P. Parys; M. Pfeifer; T. Pisarczyk; K. Rohlena; M. Rosinski; L. Ryć; J. Skala; L. Torrisi; J. Ullschmied; A. Velyhan; J. Wolowski

Intense laser-beam interactions with preformed plasma, preceding the laser-target interactions, significantly influence both the ion and X-ray generation. It is due to the laser pulse (its total length, the shape of the front edge, its background, the contrast, the radial homogeneity) as well as plasma (density, temperature) properties. Generation of the superfast (FF) ion groups is connected with a presence of non-linear processes. Saturated maximum of the charge states (independently on the laser intensity) is ascribed to the constant limit radius of the self-focused laser beam. Its longitudinal structure is considered as a possible explanation of the course of some experimental dependencies obtained.


IEEE Transactions on Plasma Science | 2006

Neutron Emission Characteristics of Pinched Dense Magnetized Plasmas

Hellmut Schmidt; P. Kubes; Marek J. Sadowski; M. Scholz

One outstanding property of pinch plasmas (Z-pinch, plasma focus, capillary discharge) is the generation of intensive very high energy electron and ion beams caused by high-amplitude electromagnetic fields. High-temperature dense magnetized plasmas are produced in high-current electrical discharges of various geometries by fast magnetic and shock compression. If the discharge is operated in deuterium gas, fusion reactions take place. It has been found from neutron emission characteristics that most of the fusion reactions are from the beam target and not from thermonuclear processes. Ion trajectories within and outside the plasma can be described by a generalized gyrating particle model (GPM). The results of space-, time-, and energy-resolved measurements of fusion neutrons (2.45 MeV) and protons (3 MeV), obtained from a 500-kJ plasma focus, are presented. Results are interpreted based on the GPM


international free electron laser conference | 2003

Ablation of various materials with intense XUV radiation

L. Juha; J. Krása; Andrea Cejnarova; Dagmar Chvostova; V. Vorlicek; J. Krzywinski; R. Sobierajski; Andrzej Andrejczuk; M. Jurek; D. Klinger; Henryk Fiedorowicz; A. Bartnik; M. Pfeifer; Pavel Kubát; Ladislav Pina; Jozef Kravarik; P. Kubes; Yuri L. Bakshaev; Valeri D. Korolev; Andrei S. Chernenko; Mikhail I. Ivanov; M. Scholz; L. Ryć; Josef Feldhaus; J. Ullschmied; F. P. Boody

Ablation behavior of organic polymer (polymethylmethacrylate) and elemental solid (silicon) irradiated by single pulses of XUV radiation emitted from Z-pinch, plasma-focus, and laser-produced plasmas was investigated. The ablation characteristics measured for these plasma-based sources will be compared with those obtained for irradiation of samples with XUV radiation generated by a free-electron laser.


IEEE Transactions on Plasma Science | 2010

Transformation of the Pinched Column at a Period of the Neutron Production

P. Kubes; M. Paduch; T. Pisarczyk; M. Scholz; D. Klir; Jozef Kravarik; K. Rezac; T. Chodukowski; I. Ivanova-Stanik; L. Karpinski; E. Zielinska; Krzysztof Tomaszewski; Marek J. Sadowski

A PF-1000 device working with a deuterium gas filling and a current on the order of 1 MA was used for studies of the pinch-column structure by means of a laser interferometric system at a period of hard X-ray (HXR) and neutron production. Three different phases of the plasma-column evolution, corresponding to the intense HXR and neutron emission, were studied for discharges with neutron yields equal to about 1011 neutrons/shot. First, the start of the stagnation of a pinch column was considered; as the second phase, the development and disruption of constrictions was studied, and as the third phase, the decrease of the plasma density in a part of the plasma column during its stagnation was considered. Regions of the probable electron and ion acceleration and possible neutron production were identified.


IEEE Transactions on Plasma Science | 2006

Correlation of Radiation With Electron and Neutron Signals Taken in a Plasma-Focus Device

P. Kubes; Jozef Kravarik; D. Klir; K. Rezac; M. Scholz; M. Paduch; Krzysztof Tomaszewski; I. Ivanova-Stanik; Barbara Bienkowska; L. Karpinski; Marek J. Sadowski; Hellmut Schmidt

In the PF 1000 plasma-focus device, deuterium is used as a filling gas for the study of fast neutrons (originated from D-D fusion reactions) and X-rays. The X-ray signals have two peaks. The first peak corresponds to the time of the minimum diameter of the pinch phase, as recorded by the visible frames. The second peak has its maximum 150 to 200 ns later. The electrons with energy above a few hundreds of kiloelectronvolts are registered mostly at the first peak in both axial directions. Upstream and downstream electrons differ in their intensity (ratio 3 : 1), temporal profile, and time of their maximum. The energy of the neutrons and the time of their generation are determined by the time-of-flight method using six or seven scintillation detectors positioned in the axial direction. Each neutron pulse has a dominant portion of beam-target origin with downstream energies up to 3.2 MeV and the final portion of the neutrons with energies in the range of 2.2 to 2.7 MeV. The evolution of the neutron pulses correlates with the visible frames. The first pulse correlates with the fast downstream motion of the intense radiating axis layer of the pinch and with the forming and existence of the radiating ball-shaped structure at the bottom of the dilating plasma sheath. The second neutron pulse correlates with the exploding of the plasma after the second pinching, and with the forming and existence of the structure of the dense plasma at the bottom of the dilating current sheath, which is similar to the first pulse


Physics of Plasmas | 2014

Filamentary structure of plasma produced by compression of puffing deuterium by deuterium or neon plasma sheath on plasma-focus discharge

P. Kubes; M. Paduch; J. Cikhardt; Jiri Kortanek; B. Cikhardtova; K. Rezac; D. Klir; J. Kravarik; E. Zielinska

The present experiments were performed on the PF-1000 plasma focus device at a current of 2 MA with the deuterium injected from the gas-puff placed in the axis of the anode face. The XUV frames showed, in contrast with the interferograms, the fine structure: filaments and spots up to 1 mm diameter. In the deuterium filling, the short filaments are registered mainly in the region of the internal plasmoidal structures and their number correlates with the intensity of neutron production. The longer filamentary structure was recorded close to the anode after the constriction decay. The long curve-like filaments with spots were registered in the big bubble formed after the pinch phase in the head of the umbrella shape of the plasma sheath. Filaments can indicate the filamentary structure of the current in the pinch. Together with the filaments, small compact balls a few mm in diameter were registered by both interferometry and XUV frame pictures. They emerge out of the dense column and their life-time can be greater than hundreds of ns.


Physics of Plasmas | 2012

Deuterium gas puff Z-pinch at currents of 2 to 3 mega-ampere

D. Klir; A. V. Shishlov; P. Kubes; K. Rezac; F. I. Fursov; V. A. Kokshenev; B.M. Kovalchuk; J. Kravarik; N. E. Kurmaev; A Yu Labetsky; N. A. Ratakhin

Deuterium gas-puff experiments have been carried out on the GIT-12 generator at the Institute of High Current Electronics in Tomsk. The emphasis was put on the study of plasma dynamics and neutron production in double shell gas puffs. A linear mass density of deuterium (D2) varied between 50 and 85 μg/cm. Somewhat problematic was a spread of the D2 gas at a large diameter in the central anode–cathode region. The generator operated in two regimes, with and without a plasma opening switch (POS). When the POS was used, a current reached a peak of 2.7 MA with a 200 ns rise time. Without the POS, a current rise time approached 1500 ns. The influence of different current rise times on neutron production was researched. Obtained results were important for comparison of fast deuterium Z-pinches with plasma foci. Average DD neutron yields with and without the POS were about 1011. The neutron yield seems to be dependent on a peak voltage at the Z-pinch load. In all shots, the neutron emission started during stagnat...


Review of Scientific Instruments | 2014

Measurement of the target current by inductive probe during laser interaction on terawatt laser system PALS

J. Cikhardt; J. Krása; M. De Marco; M. Pfeifer; A. Velyhan; E. Krouský; B. Cikhardtova; D. Klir; K. Řezáč; J. Ullschmied; J. Skala; P. Kubes; J. Kravarik

Measurements of the return-current flowing through a solid target irradiated with the sub-nanosecond kJ-class Prague Asterix Laser System is reported. A new inductive target probe was developed which allows us measuring the target current derivative in a kA/ns range. The dependences of the target current on the laser pulse energy for cooper, graphite, and polyethylene targets are reported. The experiment shows that the target current is proportional to the deposited laser energy and is strongly affected by the shot-to-shot fluctuations. The corresponding maximum target charge exceeded a value of 10 μC. A return-current dependence of the electromagnetic pulse produced by the laser-target interaction is presented.

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D. Klir

Czech Technical University in Prague

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J. Kravarik

Czech Technical University in Prague

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K. Rezac

Czech Technical University in Prague

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M. Scholz

Polish Academy of Sciences

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J. Cikhardt

Czech Technical University in Prague

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Jozef Kravarik

Czech Technical University in Prague

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L. Karpinski

Military Technical Academy

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B. Cikhardtova

Czech Technical University in Prague

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J. Krása

Academy of Sciences of the Czech Republic

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Jiri Kortanek

Czech Technical University in Prague

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